Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Particle of energy

The energy of the y-rays is indicative of the isotope present, and the intensity of the y-rays is a measure of the concentration of the isotope in the sample. The limitation of this method is that, in order to have a nuclear reaction, the repulsive Coulomb barrier has to be overcome. For incident particles of energy up to 3 MeV, the only accessible elements are the light elements with Z< 15 the cross-sections of the remaining elements become rapidly negligible. [Pg.107]

If the target is irradiated with particles of energy greater than there will be a defined depth below the surface where f a reaches fiar The corresponding Eb values may be calculated, and corrected for the energy loss in the outgoing direction on its way to the detector. [Pg.118]

It should be noted that each factorial appearing in the denominator of Eq. (24) arises from the permutation of the b identical particles of energy e,. [Pg.342]

Alpha particles are composed of two protons and two neutrons. Thus they have Z = 2, N = 2, and A = 4 and correspond to a helium nucleus He. The emission of a particles thus produces a decrease of 4 units in A. An unstable nuclide undergoing a decay may emit a particles of various energy and thus directly reach the ground level of the stable product. Alternatively, as in )3 emission, an intermediate excited state is reached, followed by y emission. Figure 11.7 shows, for example, the decay process of ioTh., which may directly attain the ground level of by emission of a particles of energy 5.421 MeV or intermediate excited states by emission of a particles of lower energy, followed by y emission. [Pg.720]

Figure E.5 Schematic diagram of a particle of energy E incident on a barrier of height V0 and thickness L. The wave function v(j is also shown. Figure E.5 Schematic diagram of a particle of energy E incident on a barrier of height V0 and thickness L. The wave function v(j is also shown.
These facts were explained by Einstein5 in 1905 in a way that now appears very simple, but in fact relies on concepts that were at the time revolutionary. Einstein went beyond Planck and postulated that not only was the process of absorption and emission of light quantized, but that light itself was quantized, consisting in effect of particles of energy... [Pg.90]

In spectroscopy it is useful to consider the propagation of electromagnetic radiation in a quantitative manner. Light is transmitted as discrete packets or as a stream of particles of energy called photons. These photons have a specific energy and for spectroscopy are quantized and described by the following equation ... [Pg.101]

It is clear that the introduction of a critical volume fraction is a step toward dealing with percolation on a continuum. To this end Zallen and Scher (1971) considered the motion of a classical particle in a random potential, V r), and introduced a function, which detines the fraction of space accessible to particles of energy E. The connection with percolation is in the fact that, for energies such that 4>(E) > c(.E), there are infinitely extended volumes of allowed (V < T) space. The critical value c is identified with 0.15 for d = 3, and delocalized states appear above c ... [Pg.157]

Nearly 100% of all these decay processes correspond to p-Particles of energy 0.61 MeV and y-Radiations of energy 0.364 MeV. The decay to form stable nuclides may involve the formation of many unstable intermediate radionuclides. For example, the decay of 5oSn to 53 , shown below, involves the formation of a number of intermediate nuclides ... [Pg.3084]

Ei>E2) arrives to the Earth first, N2(Ej) are doublets whose particle of energy Ei arrives second. [Pg.344]

Equation (4.10) defines the total collision cross-section, cr(E). between an energetic particle of energy E and the target atoms. The total cross-section gives a measure of the probability for any type of collision to occur where energy-transfers are possible, for energies up to and including the maximum value... [Pg.43]

In 1897, Thomson announced that cathode rays are streams of negative particles of energy. These particles are electrons. Similar experiments, conducted by Goldstein, led to the discovery of particles that are equal in charge to the electron but opposite in sign. These particles, much heavier than electrons (actually 1837 times as heavy), are called protons. [Pg.47]

Bose-Einstein distribution - A modification of the Boltzmann distribution which applies to a system of particles that are bosons. The number of particles of energy E is proportional to [e<, where g is a normalization constant, k is the... [Pg.98]

What is the exact nature of light Does it consist of waves or is it a stream of particles of energy It seems to be both (see Figure 11.5). This situation is often referred to as the wave-particle nature of light. [Pg.363]


See other pages where Particle of energy is mentioned: [Pg.686]    [Pg.24]    [Pg.2]    [Pg.359]    [Pg.53]    [Pg.419]    [Pg.9]    [Pg.26]    [Pg.236]    [Pg.345]    [Pg.42]    [Pg.205]    [Pg.345]    [Pg.31]    [Pg.307]    [Pg.2]    [Pg.322]    [Pg.436]    [Pg.587]    [Pg.2]    [Pg.336]    [Pg.25]    [Pg.260]    [Pg.96]    [Pg.547]    [Pg.547]    [Pg.86]    [Pg.225]    [Pg.360]    [Pg.96]   
See also in sourсe #XX -- [ Pg.31 ]

See also in sourсe #XX -- [ Pg.2 ]




SEARCH



Analysis of charged particles for charge, mass and energy

Atomic Particles, Photons and the Quantization of Electron Energies Heisenbergs Uncertainty Principle

Bombardment of nuclei by high-energy a-particles and neutrons

Characteristics of Type I ELM Energy and Particle Losses from the Core Plasma

Dissolution dispersal of particle energy

Electron energy levels of adsorbed particles

Energy Levels of Charged Particles in Condensed Phases

Energy Loss in the Interaction of Atomic Particles with Solid Surfaces

Energy distribution, of sputtered particles

Energy levels of particle in a box

Energy of Particles Backscattered from Thin and Thick Targets

Energy of a particles

Energy of interaction between particles

Kinetic energy of the charged particle

Kinetic energy, of particles

Particle energy

Potential Energy of Interaction Between Particles and Surfaces

Potential energy of charged particles

Range, of high energy particles

The Potential Energy of Interaction Between Particles

The Wave-Particle Duality of Matter and Energy

© 2024 chempedia.info